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      <title-group>
        <article-title>Properties of Ma jority Transformations under Random Processes Parameters Measurement</article-title>
      </title-group>
      <contrib-group>
        <contrib contrib-type="author">
          <string-name>Elena Stepanova?</string-name>
          <xref ref-type="aff" rid="aff0">0</xref>
        </contrib>
        <contrib contrib-type="author">
          <string-name>Alexey Liagin</string-name>
          <xref ref-type="aff" rid="aff0">0</xref>
        </contrib>
        <contrib contrib-type="author">
          <string-name>Alla Pletukhina</string-name>
          <xref ref-type="aff" rid="aff0">0</xref>
        </contrib>
        <aff id="aff0">
          <label>0</label>
          <institution>North-Caucasus Federal University</institution>
        </aff>
      </contrib-group>
      <fpage>53</fpage>
      <lpage>56</lpage>
      <abstract>
        <p>Statistical inference problem arises when you want to give the best, in some sense, the answers to a limited number of observations. When it comes to problems of statistical inference, it is assumed that it is possible to obtain a random sample, is set consisting of the realizations of independent and identically distributed random variables. The article attempts to assess quality parameters of a random process normally distributed through the application of order statistics (particularly the selected median) with a limited sample size.</p>
      </abstract>
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    <sec id="sec-1">
      <title>-</title>
      <p>In practice it is often required to determine the quantitative attribute
(variables) against noise background. Lets assume that its initially known what kind
of distribution a sign exactly possesses. There comes the task of assessing
parameters that determine this distribution. If its known that the attribute under
examination is normally distributed in the entire assembly, which is typical for
mixture of signal and Gaussian noise at noise-to-signal ratio greater than unity,
it is necessary to evaluate (calculate approximately) mathematical expectation
and root-mean-square deviation, as these two parameters completely determine
normal distribution.</p>
      <p>Usually at a researchers disposal there is only sample data, e.g. quantitative
attribute values x1, x2, ..., xn received as a result of N observations (observations
assumed to be independent). Test variable is expressed in terms of this data.</p>
      <p>When considering x1, x2, ..., xn as independent random variables X1, X2, ..., Xn,
we can state that to find a statistical evaluation of the unknown parameter
theoretical distribution means to find a function of the observed random variables,
which gives an approximate value of the parameter estimated.</p>
      <p>Most frequently in practice, for equally accurate measurements, parameters
of random process distribution are evaluated by general average, which is
reasonable for a large number of values of random variables observed. However for
a small number of measurements, with high degree of unequal accuracy, as is
known from mathematical statistics, sample median estimate is more effective
than sample average.</p>
      <p>Let physical process be described as a function of time X(t). On the signal
parameter tester signal X = X(t) + n(t) is applied where X(t) - measuring
signal, n(t) - external influence (noise). Signal parameters are evaluated at a
certain time interval Δ(t).</p>
      <p>In mathematical statistics we know integrated (averaged) evaluation methods
x(Δt) = nl→im∞ iP=ni xni , where i = 1...n - equal for the majority of equally accurate
measurements from the entire assembly X(t) ⊂ f (x1, x2, ..., xn). However, these
techniques make evaluation of the random process parameters consistent,
unbiased and effective only under controlled (predictable) changes of the parameters
of random process.</p>
      <p>When changes of random process parameters are unpredictable
nonparametric method for estimation of the process parameters is interesting. Its principle
is as follows: in the measurement time interval Δ(t) several measurements of
the random process parameter xj = x + xj (j = 1...k) are made. Sensor
output signals contain nj measurement random errors caused by external influences
(noise) which properties are characterized by probability densities (fj (x))
Results of measurements (random variables xj ) form set of variate values
x1, x2, ..., xk
so that x1 &lt; x2 &lt; ... &lt; xk. In case of odd number of measurements (K = 2k + 1)
mean proportional of set of variate values (1.4.2) is taken as valuation of Z
parameter of the process measured.</p>
      <p>
        Z = X(k + 1)
(
        <xref ref-type="bibr" rid="ref2">2</xref>
        )
(
        <xref ref-type="bibr" rid="ref1">1</xref>
        )
(
        <xref ref-type="bibr" rid="ref3">3</xref>
        )
      </p>
      <p>For sample size K = 2k + 1 = 3 suggested measurement algorithm can
be implemented on (max and min) transformations. Then mathematical model
and algorithm of measurement can be represented as Z = med(x1, x2, x3) =
max{min(x1, x2), min(x1, x3), min(x2, x3}</p>
      <p>
        For symmetrically distributed measurement errors estimate (
        <xref ref-type="bibr" rid="ref2">2</xref>
        ) is unbiased.
Obviously, the error of estimate (
        <xref ref-type="bibr" rid="ref2">2</xref>
        ) is equal to the errors median nj
e = Z − x = n(k + 1)
      </p>
      <p>For practice, a case is important when the distribution of measurement errors
on the observation interval is different, the differences characteristics are not
known beforehand and cannot be used for optimal algorithms measurements
apply. This situation occurs while the rapid changes in the measured parameter
of physical process on the observation interval, for example, rapid changes in the
amplitude of the analog signal, the frequency alteration and phase of harmonic
oscillations - the information carriers in a rapidly changing interference intensity
on the observation interval and a number of other situations.</p>
      <p>Lets compare by statistical efficiency and estimation accuracy of the physical
parameter process on sample median with a simple averaging for the case of
unequal dimensions.</p>
      <p>For practice, a case is interesting when the sample size for the measurement
interval K = 3, the measurement errors are normally distributed with zero mean
and variances σ2, σ22, σ32 and it is unknown, what specific measurement
corre1
sponds to a certain level of error.</p>
      <p>Elena Stepanova, Alexey Liagin, and Alla Pletukhina</p>
      <p>
        According to [1], the probability density estimation errors algorithm sample
median:
(
        <xref ref-type="bibr" rid="ref4">4</xref>
        )
At a normal distribution inaccuracy, the formula looks like this:
Fi(x) = 0, 5 1 + erf
      </p>
      <p>x
√2σi
, where erf (y) = √</p>
      <p>e−t2 dt.</p>
      <p>y
2 Z
π
0</p>
      <p>Error variance σ22 for the sample median, the corresponding distribution (5)
turns out to be [1]</p>
      <p>From (6) follows that if the error variance of any two measurements are
limited and the errors of the third dimension are infinitely large variance, and
the measurement results practically unreliable, error variance is found to be
σ22 = 21 (σ12 + σ22).</p>
      <p>This means that the assessment on sample median virtually eliminated false
data.</p>
      <p>The other situation is observed at an average measurement results. The
calculation is defined as:</p>
      <p>That is: an unlimited increase of dispersion errors in one of the measurements
leads to unlimited increase of error variance estimates.</p>
      <p>At symmetric distribution laws Fi(x) of errors and when they do not contain
systematic components, the probability P (Δ) in the case of unequal probability
measurement is defined as:
1
P (Δ) = F1(Δ)F2(Δ)+F1(Δ)F3(Δ)+F2(Δ)F3(Δ)−2F1(Δ)F2(Δ)F3(Δ)− 2 (7)</p>
      <p>1 Δ
P (Δ) = 1 − 2 Φ √2σδ
1 − Φ2
,
(8)
where δ = σσ3 .</p>
      <p>when unequal measurements, the sample median has the best performance in
terms of quality considered criterion than the sample mean an order of magnitude
or more. This demonstrates the feasibility of applying the algorithm sample
median for measuring the parameters of stochastic processes on the background
noise and the impact of external influences, both on a physical process, and the
measuring device. Practical confirmation the latest are researches for example,
in [2,3,4].</p>
    </sec>
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